Natural Gas Isobaric Liquefaction Apparatus

ABSTRACT

This invention is about a natural gas isobaric liquefaction apparatus, which is based on the Rankine cycle system of similar thermal energy power circulation apparatus at cryogenic side, a cryogenic liquid pump is used to input power and the refrigerating media makes up cold to the natural gas liquefying apparatus, so as to realize the isobaric liquefaction of natural gas. The natural gas liquefying apparatus of this invention can save energy by over 30% as compared with the traditional advanced apparatus with the identical refrigerating capacity, therefore it constitutes a breakthrough to the traditional natural gas liquefaction technology, with substantial economic, social and environmental protection benefits.

TECHNICAL FIELD

This invention is about a natural gas isobaric liquefaction apparatus,specifically in the technical field of cryogenic refrigeration.

BACKGROUND OF THE INVENTION

Natural gas is a high quality and clean petrochemical energy, with aquite important position in national economy. The liquefaction andstorage of natural gas is a critical technology in its development andutilization, it has become an industry both at home and overseas, andgrows at an average annual rate of 8%, in recent years, it has beengrowing quite rapidly in the energy consumption pattern of China. Thetechnology to liquefy natural gas has become a high technology, beingattached with importance by more and more scientific and technologicalsectors.

It is expected that by the mid of this century, if China consumesnatural gas of 5000*10⁸ m³/a, including import of LNG1000*10⁸ m³/a(equivalent the present import of Japan), the usable cold energy is257*10⁸ kWh/a, equivalent to the annual power generation amount of apower plant of 600*10⁴ kW. Therefore, it is worth our in-depthconsideration on how to realize breakthroughs in aspects of technology,management mechanism and market operation for LNG, to substantiallyreduce the energy consumption for LNG, push forward rapid development oflarge scale cold energy industrial chain including air separation andgasification of coal with enriched air for huge energy conservation andeconomic benefit, so as to make contribution to the full realization ofcyclic economy and saving economy in China. In the meantime, the rapiddevelopment and transition of Chinese economy has determined theabsolute necessity of large-scale use of LNG, and also provided a hugeuser market.

Traditional natural gas liquefaction is mainly based on the followingthree processes:

1. Cascade liquefying process (also referred to as step liquefactionprocess, overlapped liquefying process or serial vaporization andcondensation liquefying process), mainly applied in natural gasliquefying apparatus carrying basic loads;

2. Mixed refrigerant liquefying process:the so-called MRC liquefyingprocess, is a process in which a medium of mixed refrigerant withmulti-components including hydrocarbon compound of C1 to C5 and N_(2,)is condensed, vaporized and throttle expanded to obtain a certainrefrigerating capacity at different temperature level so as torefrigerate and liquefy natural gas step by step. MRC has achieved thepurpose similar to cascade liquefying process, and also overcome itsdisadvantage of complicated system. Since the 1980s, almost all newlybuilt and expanded natural gas liquefaction apparatus for basic loadsare based on the liquefying process with propane precooling mixedrefrigerant;

3. Liquefying process with expander: this process is based on the Claudecycle of refrigerant in a turbine expander, to realize liquefaction ofnatural gas. When the gas expands and makes work in an expander, thetemperature is lowered and power recovered. Depending on differentrefrigerant, it can be classified as nitrogen expansion liquefyingprocess and natural gas expansion liquefying process. These processeshave the advantages: (1) simple process, flexible regulation, reliableworking, easy startup and operation, and convenient maintenance; and (2)with the natural gas itself used as medium, it can save the expense ofproduction, transport and storage of refrigerant. The disadvantages are:(1) all gas streams to the apparatus requires in-depth drying; (2) thereflux pressure is low, the area of heat exchange is large and the inputof equipment metal is high; (3) it is restricted by the number of LPusers; (4) the liquefaction rate is low, if re-circulation is required,the power consumption will increase greatly when additional circulationcompressors are used. A liquefying process with expander is easy tooperate with moderate investment, and is particularly suitable to peakregulation type natural gas liquefaction apparatus with fairly lowcapacity.

FIG. 1 is a schematic diagram of cascade natural gas liquefying process.

FIG. 2 is a schematic diagram of APCI propane precooling mixedrefrigerant liquefying process.

FIG. 3 shows the natural gas expansion liquefying process, in which:1—dehydrating agent, 2—carbon dioxide removal column, 3—water cooler,4—returns to the gas compressor, 5, 6, 7—heat exchangers, 8—subcooler,9—tank, 10—expander, 11—compressor.

FIG. 4 shows the nitrogen expansion liquefying process, in which:1—pre-treatment apparatus, 2, 4, 5—heat exchanger, 3—heavy hydrocarbonseparator, 6—nitrogen stripper, 7—turbine expander, 8—nitrogen-methaneseparating column, 9—circulation compressor.

FIG. 5 is a schematic diagram of natural gas expansion liquefyingprocess with propane precooling, in which: 1, 3, 5, 6, 7—heatexchangers, 2, 4—propane heat exchangers, 8—water cooler, 9—compressor,10—braking compressor, 12, 13, 14—gas-liquid separator.

The design of the afore-said traditional natural gas liquefyingprocesses is mainly based on the theoretical foundation ofthermodynamics, Carnot reverse cycle of identical temperature differenceis used to analyze the natural gas liquefying process, the economicindicator of the cycle is the refrigeration coefficient, or the ratio ofobtained gain to the cost of consumption, and also, of all refrigeratingcycles between atmospheric environment with temperature of T₀ and lowtemperature heat source with temperature of Tc (such as refrigerationstore), the reverse Carnot cycle has the highest refrigerationcoefficient:

$\begin{matrix}{ɛ_{c} = {({COP})_{R,C} = {\frac{q_{2}}{w_{0}} = \frac{T_{c}}{T_{0} - T_{c}}}}} & (1)\end{matrix}$

In the formula above, ε_(c) is the refrigeration coefficient, q₂refrigerating capacity of the cycle, and w₀ the net work consumed by thecycle.

The actual cycle efficiency is usually described by the ratio ofrefrigeration coefficient of actual cycle and theoretical cyclingrefrigeration coefficient, however, its theoretical basis is cyclicanalysis of refrigerating process with Carnot reverse cycle.

In fact, in his thesis “Reflections on the Motive Power of Heat”, Carnotconcluded that: of all heat engines working between two constanttemperature heat sources of different temperatures, the reversible heatengine has the highest efficiency.” This was later referred to as theCarnot theorem, after rearranging with the ideal gas state equation, thethermal efficiency of Carnot cycle obtained is:

$\begin{matrix}{\eta_{c} = {1 - \frac{T_{2}}{T_{1}}}} & (2)\end{matrix}$

In Formula (2), temperature T₁ of the high temperature heat source andtemperature T₂ of low temperature heat source are both higher than theatmosphere ambient temperature T₀, and the following importantconclusions can be obtained:

1) The thermal efficiency of Carnot cycle only depends on thetemperature of high temperature heat source and low temperature heatsource, or the temperature at which the media absorbs heat and releaseheat, therefore the thermal efficiency can be increased by increasing T₁and T₂.

2) The thermal efficiency of Carnot cycle can only be less than 1, andcan never be equal to 1, because it is not possible to realize T₁=∞ orT₂=0. This means that a cyclic engine, even under an ideal condition,cannot convert all thermal energy into mechanical energy, of course, itis even less possible that the thermal efficiency is greater than 1.

3) When T₁=T₂, the thermal efficiency of the cycle is equal to 0, itindicates that in a system of balanced temperature, it is not possibleto convert heat energy into mechanical energy, heat energy can producepower only with a certain temperature difference as a thermodynamiccondition, therefore it has verified that it is not possible to build amachine to make continuous power with a single heat source, or theperpetual motion machine of the second kind does not exist.

4) Carnot cycle and its thermal efficiency formula are of importantsignificance in the development of thermodynamics. First, it laid thetheoretical foundation for the second law of thermodynamics; secondly,the research of Carnot cycle made clear the direction to raise theefficiency of various heat power engines, i.e. increasing the heatabsorbing temperature of media and lowering the heat release temperatureof media as much as possible, so that the heat is release at the lowesttemperature that can be naturally obtained, or at the atmospherictemperature. The method mentioned in Carnot cycle to increase the gasheat absorbing temperature by adiabatic compression is still a generalpractice in heat engines with gas as media today.

5) The limit point of Carnot cycle is atmospheric ambient temperature,and for refrigerating process cycles below ambient temperature, Carnotcycle has provided no definite answer.

However, the basic theory of thermodynamics cannot make simple, clearand intuitional explanation of the cycling process of natural gasliquefying apparatus, to produce 1 ton of LNG, the power consumption ofequipment and utilities is about 850 kWh, which means very high energyconsumption in the process.

Einstein commented the classical thermodynamics this way: “A theory willgive deeper impression to the people with simpler prerequisite, moreinvolvement and wider scope of application.” In the exploration of basictheory in the refrigeration field, this point should be inherited andcarried forward.

Therefore, it has become a difficult issue in the research of naturalgas liquefaction technical field to research on the natural gasliquefaction cycles, to really find the theoretical foundation for therefrigerating apparatus cycle and the correct direction to improve theprocess, and to organize new natural gas liquefying apparatus process onthis foundation and substantially reduce the energy consumption ofnatural gas liquefying apparatus.

CONTENT OF THE INVENTION

The purpose of this invention is to improve the theoretical analysis ofCarnot theorem when applied to natural gas liquefying apparatus cycle,propose the new refrigerating theory corresponding to thermodynamictheory, i.e. the cold dynamics theory, and also propose a new naturalgas isobaric liquefaction apparatus designed by applying this principle,to overcome the disadvantages of traditional natural gas liquefyingprocess such as complicated process, high energy consumption and massiveutility facilities such as circulating cooling water system, whileretaining and further developing the advantages such as liquefyingprocess with expander, so that energy consumption can be substantiallycut by over 30%, and also realize isobaric condensation of natural gas,and also greatly reducing equipment maintenance and materials backup, soas to realize the transformation of natural gas liquefaction technology.

Corresponding to the traditional scope of thermodynamics, the basicconcept of cold dynamics is proposed: any environment below theatmospheric ambient temperature is referred to as a cold source,corresponding to heat source above the ambient temperature; andcorresponding to heat energy and heat, the corresponding concepts ofcold energy and cold are proposed; the said refrigerating apparatusrefers to that consuming mechanical power to realize transfer of coldenergy from atmospheric environment to cryogenic cold source or from acold source of low temperature to that of lower temperature. In thetransfer of cold energy, some substance is required as working media inthe refrigerating apparatus, and it is referred to as refrigeratingmedia.

In the refrigerating process, the transfer of cold energy follows theenergy conversion and conservation law.

To describe the cold transfer direction, conditions and limit in therefrigerating process, the second law of cold dynamics is proposed: theessence of the second law of cold dynamics is identical to that of thesecond law of thermodynamics, and it also follows the “energy qualitydeclining principle”, i.e. cold energy of different forms differs in“quality” in the ability to convert into power; and even the cold energyof the same form also has different ability of conversion at differentstatus of existence. All actual processes of cold energy transfer arealways in the direction of energy quality declination, and all coldenergy spontaneously converts in the direction of atmosphericenvironment. The process to increase the quality of cold energy cannotperform automatically and independently, a process to increase energyquality is surely accompanied by another process of energy qualitydeclination, and this energy quality declination process is thenecessary compensating condition to realize the process to increaseenergy quality, that is, the process to increase energy quality isrealized at the cost of energy quality declination as compensation. Inthe actual process, the energy quality declination process, as a cost,must be sufficient to compensate for the process to increase the energyquality, so as to meet the general law that the total energy qualitymust certainly decline. Therefore, with the given compensation conditionfor energy quality declination, the process to increase the energyquality surely has a highest theoretical limit. This theoretical limitcan be reached only under the complete reversible ideal condition, inthis case, the energy quality increase value is just equal to thecompensation value for energy quality declination, so that the totalenergy quality remains unchanged. This shows that a reversible processis a pure and ideal process of energy quality conservation, in anirreversible process, the total energy quality must surely decline, andin no case it is possible to realize a process to increase the totalenergy quality in an isolated system. This is the physical connotationof the energy quality declining principle, the essence of the second lawof cold dynamics, and also the essence of the second law ofthermodynamics, and it reveals the objective law of the direction,conditions and limit of process that must be followed by all macroscopicprocesses.

The basic formula describing the second law of cold dynamics is:

$\begin{matrix}{\eta_{c} = {1 - \frac{T_{c\; 2}}{T_{c\; 1}}}} & (3)\end{matrix}$

In Formula (3), Tc2<Tc1<T₀, T₀ is the ambient temperature, all based onKelvin temperature scale.

With respect to the ambient temperature T₀, the maximum cold efficiencyof the cold source at Tc1 and Tc2 is:

$\begin{matrix}{\eta_{c} = {1 - \frac{T_{c\; 1}}{T_{0}}}} & (4) \\{\eta_{c} = {1 - \frac{T_{c\; 2}}{T_{0}}}} & (5)\end{matrix}$

Suppose q₂ is the refrigerating capacity of the cycle, and w₀ the netpower consumed by the cycle, then when the cold source temperature isTc1:

$\begin{matrix}{w_{0} = {\left( {1 - \frac{T_{c\; 1}}{T_{0}}} \right)q_{2}}} & (6)\end{matrix}$

Similarly, when the cold source temperature is Tc2

$\begin{matrix}{w_{0} = {\left( {1 - \frac{T_{c\; 2}}{T_{0}}} \right)q_{2}}} & (7)\end{matrix}$

It is not difficult to see from Formulas (4) to (7) that, the efficiencyof the cold dynamics is between 0 and 1, and due to unavoidableirreversibility in the actual process, the refrigerating cycleefficiency is always less than 1;

When the ambient temperature T₀ is determined, the lower cold sourcetemperature, the more refrigerating capacity can be obtained with thesame amount of power input from that cold source, and this has pointedout the direction for building new natural gas liquefying apparatusprocesses.

It should be noted that:

(1) The cold is transferred spontaneously from the cryogenic cold sourceto ambient temperature;

(2) It is not possible to transfer cold from a cryogenic cold source toa cold source of lower temperature without causing other change;

(3) When the cold is transferred from a cryogenic cold source to theenvironment, the power exchanged with the outside is w₀, which includesthe useless work p₀(V₀−V_(c)) made to the environment, p₀ is theatmospheric pressure, V₀ the volume at ambient temperature, Vc thevolume at cold source temperature, and the maximum reversible usefulwork made is:

$\left( W_{n} \right)_{\max} = {{W_{0} - {p_{0}\left( {V_{0} - V_{c}} \right)}} = {{\left( {1 - \frac{Tc}{To}} \right)Q_{0}} - {p_{0}\left( {V_{0} - V_{c}} \right)}}}$

(4) When the cold is transferred from a cryogenic cold source to theenvironment, the useless energy transferred to the environment is:

$E_{useless} = {\frac{Tc}{To}Q_{0}}$

The useless work transferred to the environment is: p₀ (V₀−V_(c))

Corresponding to the useful energy “Yong” and useless energy “Jin” ofheat quantity, and with the meanings of heat for fire and cold forwater, the useful energy of cold energy is named as “cold energy lian”,and the useless energy of cold energy transferred to the environment isnamed as “cold energy jin”, and this “jin” is to water.

(5) When cold energy is transferred to environment, the best form ofmaking work to the outside is using a thermoelectric generator ofSeebeck effect, generator, or cold power generator;

(6) In cold dynamics, the energy must and also inevitably follow theenergy conversion and conservation law;

(7) With reference to the conception of finite time thermodynamics, itis possible to develop the basic theory of finite time cold dynamics;

(8) The quality of cold energy cannot be assessed by separating it fromthe specific environment;

(9) Cold dynamics and thermodynamics are two branches of the energetics,and are a unity of opposites: in a cryogenic refrigerating cycle, whilefollowing the second law of cold dynamics, the cycle process ofrefrigerant media formed in the cryogenic environment also follows theRankine cycle, so it comes back to the Carnot law, just in line with theprinciple of the Chinese traditional aesthetics that yin and yangmutually complement.

It can be seen from the view above that, the supposed cold dynamics hasa theoretical framework system symmetric to thermodynamics, so itcomplies with the basic principle of scientific aesthetics, or theprinciple of opposite and complementary symmetricity.

On the basis of the afore-said cold dynamics basic principle, thisinvention has proposed a process organization different from thetraditional natural gas liquefying apparatus, to realize isobaricliquefaction of natural gas with low energy consumption, so that theenergy consumption of the natural gas liquefying apparatus can beeffectively reduced, and the specific power consumption of natural gasis reduced to about 0.24 kW·h/kg.

The purpose of this invention is realized with the following measures:

A natural gas isobaric liquefying apparatus, which is comprised of thenatural gas pretreatment system, liquefying system, cold makeup system,storage system, control system and fire fighting system, this inventiononly presents the schematic diagram of the most important part, or theliquefying process, the part not described in detail will be configuredaccording to the traditional mature technologies, and the process stepsto realize natural gas isobaric liquefaction are as follows:

(1) The raw natural gas 1 flows via the pre-treatment apparatus 2 toremove moisture and carbon dioxide, enters the cold exchanger 3 andheavy hydrocarbon separator 4 to separate the liquid heavy hydrocarboncomponent 5, and then passes through cold exchanger 6 to become theprecooled column feeding raw gas 7;

(2) The precooled column feeding raw gas 7 enters the lower column 8,flows via condensing evaporator 9 to produce supercooled methane liquid,which flows back for rectification and isobaric condensation to produceliquefied natural gas 11 or LNG, the LNG is sent to LNG tank 12;

(3) In the condensing evaporator, the pure methane liquid 13 producedfrom isobaric condensation is led to the liquid pure methane tank 14;

(4) The cold makeup system of the said apparatus refers to the setup inwhich the liquid refrigerant 20 from refrigerant tank 19 is made into arefrigerant gas-liquid mixture 22 via the cryogenic liquid pump 21 andcold regenerator 18, and enters the upper column 10, the condensingevaporator 9 condenses the methane gas in the lower column to produceliquid methane, the column outflow cryogenic refrigerant 15 from theupper column 10 flows via the cold exchanger 6 and cold exchanger 3 tocool down the raw natural gas 1, to form the refrigerant superheatedvapor 16, which flows via the expander 17 to reduce pressure andtemperature, and returns via cold regenerator 18 and throttle valve 23,to the refrigerant tank 19, the cold quantity required by the naturalgas liquefying system is made up via condensing evaporator 9, coldexchanger 6 and cold exchanger 3, so as to form the cold dynamic cyclecircuit of the refrigerant; the pressure of the cold makeup system canbe conveniently regulated via throttle valve 23.

The braking equipment 24 of the said expander 17 refers to fan, motor,hydraulic pump or gas compressor.

The methane from the top of lower column 8 can also be directly led intoupper column 10 for washing by liquid nitrogen to produce liquid puremethane, which can be directed out from the bottom of upper column 10and sent to liquid pure methane tank 14.

The said isobaric separation refers to the process that the raw naturalgas entering the natural gas liquefying system needs not to be liquefiedwith throttling pressure reduction as in the traditional natural gasliquefying process, the incoming raw natural gas 1 is only subjected toresistance loss in the equipment and pipes along the way, so it can betaken as an isobaric liquefying process.

The said liquefying system consists of the lower column 8, condensingevaporator 9 and upper column 10, in an integrated or separatedstructure.

The said refrigerant has a boiling point lower than or equal to that ofmethane under standard atmospheric pressure, and is a mixture formed byone or a number of gases including without limitation methane, nitrogen,argon, helium and hydrogen, if safety can be ensured, gaseous or liquidhydrogen can also be used, with preference as gaseous nitrogen.

The said refrigerant tank 19 is provided with necessary thermal and coldinsulation, such as thermal isolated vacuum container, and insulationmaterials such as pearlite.

The said cold exchanger 6, cold exchanger 3 and cold regenerator 18 aretube-shell type, plate-fin, micro channel or other types of coldexchanger, their structure and cold exchange elements are identical tothe tube-shell type heat exchanger, plate-fin heat exchanger, microchannel heat exchanger in the traditional natural gas liquefyingprocess, the more precise names are used in their place only for thepurpose of corresponding to the refrigerating system.

One or a number of the said cold exchanger 3, cold exchanger 6,separator 4 and cold regenerator 18 can be provided.

The equipment and their backup systems, pipes, instruments, valves, coldinsulation and bypass facilities with regulation functions not describedin this invention shall be configured with mature technologies ofgenerally known traditional natural gas liquefying systems.

Safety and regulation and control facilities associated with the naturalgas liquefying apparatus of this invention are provided, so that theapparatus can operate economically and safely with high thermalefficiency, to achieve the goal of energy conservation, consumptionreduction and environmental protection.

The apparatus of this invention is also applicable to liquefaction ofother gases, and boiling point under standard atmospheric pressure ofthe refrigerant used is lower than or equal to that of the correspondinggas to be liquefied.

This invention has the following advantages as compared with existingtechnologies:

1. Substantial energy conservation effect: the circulating gascompressor in the traditional natural gas liquefying system cycle iscancelled, by using the property of liquid as an almost incompressiblefluid, the cryogenic liquid circulating pump is used for boosted coldmakeup, to realize the isobaric liquefaction of natural gas, it caneffectively increase the efficiency of refrigerating cycle, and comparedwith a traditional natural gas liquefying apparatus, with the samerefrigerating capacity, energy can be saved by over 30%, and comparedwith the traditional advanced processes, at least 200 kWh of power canbe saved per each ton of liquefied natural gas.

2. LNG or liquid pure methane produced by isobaric condensation, cansave the electric power consumed in the traditional boosting process forLNG or pure liquid methane.

3. The gas compression work in the traditional natural gas liquefyingprocess can be saved by liquefying natural gas at low pressure and thenincreasing pressure for liquefied natural gas, so that power consumptionof the utilities associated with the natural gas liquefying system cabbe cut by over 80%.

4. Simpler process flow setup can bring into full play the potential ofthe liquefying system, and the operation can be more flexible and moreconvenient in regulation.

5. The equipment and materials inventory can be substantially reduced.

6. It can fully replace the traditional mainstream natural gasliquefying apparatus of basic loads such as propane precooling mixedrefrigerant liquefying process, becoming the prevailing process fornatural gas liquefying apparatus of both base type and peak regulationtype.

DESCRIPTION OF FIGURES

FIG. 1 is a schematic diagram of cascade natural gas liquefying process;

FIG. 2 is a schematic diagram of APCI propane precooling mixedrefrigerant liquefying process;

FIG. 3 shows the natural gas expansion liquefying process:

In FIG. 3: 1—dehydrating agent, 2—carbon dioxide removal column, 3—watercooler, 4—returns to the gas compressor, 5, 6, 7—heat exchangers,8—subcooler, 9—tank, 10—expander, 11—compressor.

FIG. 4 shows the nitrogen gas expansion liquefying process:

In FIG. 4: 1—pre-treatment apparatus, 2, 4, 5—heat exchanger, 3—heavyhydrocarbon separator, 6—nitrogen stripper, 7—turbine expander,8—nitrogen-methane separating column, 9—circulation compressor.

FIG. 5 is a schematic diagram of natural gas expansion and liquefyingprocess with propane precooling:

In FIG. 5: 1, 3, 5, 6, 7—heat exchangers, 2, 4—propane heat exchangers,8—water cooler, 9—compressor, 10—braking compressor, 12, 13,14—gas-liquid separators.

FIG. 6 is a schematic diagram of a natural gas isobaric liquefyingapparatus of this invention:

In FIG. 6: 1—raw natural gas, 2—pretreatment apparatus, 3—coldexchanger, 4—heavy hydrocarbon separator, 5—liquid heavy hydrocarboncomponent , 6—cold exchanger, 7—precooled column feeding raw gas,8—lower column, 9—condensing evaporator, 10—upper column, 11—LNG, 12—LNGtank, 13—pure liquid methane, 14—pure liquid methane tank, 15—columnoutflow cryogenic refrigerant, 16—refrigerant superheated vapor,17—expander, 18—cold regenerator, 19—refrigerant tank, 20—liquidrefrigerant, 21—cryogenic liquid pump, 22—refrigerant gas-liquidmixture, 23—throttle valve, 24—braking equipment.

EMBODIMENTS

In the following, this invention is further described in detail inconjunction with figures and embodiments.

Embodiment 1

As shown in FIG. 6, a natural gas isobaric liquefying apparatus, withnitrogen gas as refrigerant, with the specific embodiment as follows:

(1) The raw natural gas 1 flows via the pre-treatment apparatus 2 toremove moisture and carbon dioxide, enters the cold exchanger 3 andheavy hydrocarbon separator 4 to separate the liquid heavy hydrocarboncomponent 5, and then passes through cold exchanger 6 to become theprecooled column feeding raw gas 7;

(2) The precooled column feeding raw gas 7 enters the lower column 8,flows via condensing evaporator 9 to produce supercooled methane liquid,which flows back for rectification and isobaric condensation to produceliquefied natural gas 11 or LNG 1, the LNG is sent to LNG tank 12;

(3) In the condensing evaporator, the pure methane liquid 13 producedfrom isobaric condensation is led to the liquid pure methane tank 14;

(4) The liquid refrigerant 20 from refrigerant tank 19 is made into arefrigerant gas-liquid mixture 22 via the cryogenic liquid pump 21 andcold regenerator 18, and enters the upper column 10, the condensingevaporator 9 condenses the methane gas in the lower column to produceliquid methane, the column outflow cryogenic refrigerant 15 from theupper column 10 flows via the cold exchanger 6 and cold exchanger 3 tocool down the raw natural gas 1, to form the refrigerant superheatedvapor 16, which flows via the expander 17 to reduce pressure andtemperature, and returns via cold regenerator 18 and throttle valve 23,to the refrigerant tank 19, the cold quantity required by the naturalgas liquefying system is made up via condensing evaporator 9, coldexchanger 6 and cold exchanger 3, so as to form the cold dynamic cyclecircuit of the refrigerant; the pressure of the cold makeup system canbe conveniently regulated via throttle valve 23.

The braking equipment 24 of the said expander 17 is gas compressor,which is used to boost the raw natural gas.

The said refrigerant tank 19 is provided with necessary thermal and coldinsulation, such as thermal isolated vacuum container, and insulationmaterials such as pearlite.

The equipment and their backup systems, pipes, instruments, valves, coldinsulation and bypass facilities with regulation functions not describedin this invention shall be configured with mature technologies ofgenerally known traditional natural gas liquefying systems.

Safety and regulation and control facilities associated with the naturalgas liquefying apparatus of this invention are provided, so that theapparatus can operate economically and safely with high thermalefficiency, to achieve the goal of energy conservation, consumptionreduction and environmental protection.

This invention has been made public with an optimum embodiment as above,however, it is not used to restrict this invention, all variations ordecorations made by those familiar with this technology withoutdeviating from the spirit and scope of this invention also falls intothe scope of protection of this invention. Therefore, the scope ofprotection of this invention shall be that defined by the claims in thisapplication.

1. A natural gas isobaric liquefaction apparatus, this apparatusconsists of the natural gas pretreatment system, precooling system,liquefying system, cold makeup system, storage system, control systemand fire fighting system, with the features that: The cold makeup systemof the said apparatus refers to the setup in which the liquidrefrigerant (20) from refrigerant tank (19) is made into a refrigerantgas-liquid mixture (22) via the cryogenic liquid pump (21) and coldregenerator (18), and enters the upper column (10), in the condensingevaporator (9) it condenses the methane gas in the lower column (8) toproduce liquid methane, or condense the methane pumped from the lowercolumn (8) into the upper column to form liquid methane, the columnoutflow cryogenic refrigerant (15) from the upper column (10) flows viathe cold exchanger (6) and cold exchanger (3) to cool down the rawnatural gas (1), to form the refrigerant superheated vapor (16), whichflows via the expander (17) and cold regenerator (18), and returns tothe refrigerant tank (19), so as to form the cold dynamic cycle circuitof the refrigerant.
 2. The apparatus as described in claim 1, with thefeatures that: It is provided with throttle valve (23): The liquidrefrigerant (20) from refrigerant tank (19) is made into a refrigerantgas-liquid mixture (22) via the cryogenic liquid pump (21) and coldregenerator (18), and enters the upper column (10), in the condensingevaporator (9) it condenses the methane gas in the lower column (8) toproduce liquid methane, or condense the methane pumped from the lowercolumn (8) into the upper column to form liquid methane, the columnoutflow cryogenic refrigerant (15) from the upper column (10) flows viathe cold exchanger (6) and cold exchanger (3) to cool down the rawnatural gas (1), to form the refrigerant superheated vapor (16), whichflows via the expander (17), cold regenerator (18) and throttle valve(23), and returns to the refrigerant tank (19), so as to form the colddynamic cycle circuit of the refrigerant.
 3. The apparatus as describedin claim 1, with the features that: The braking equipment (24) of thesaid expander (17) refers to fan, motor, hydraulic pump or gascompressor.
 4. The apparatus as described in claim 2, with the featuresthat: The braking equipment (24) of the said expander (17) refers tofan, motor, hydraulic pump or gas compressor.
 5. The apparatus asdescribed in claim 1, with the features that: The said liquefying systemconsists of the lower column (8), condensing evaporator (9) and uppercolumn (10), in an integrated or separated structure.
 6. The apparatusas described in claim 2, with the features that: The said liquefyingsystem consists of the lower column (8), condensing evaporator (9) andupper column (10), in an integrated or separated structure.
 7. Theapparatus as described in claim 3, with the features that: The saidliquefying system consists of the lower column (8), condensingevaporator (9) and upper column (10), in an integrated or separatedstructure.
 8. The apparatus as described in claim 4, with the featuresthat: The said liquefying system consists of the lower column (8),condensing evaporator (9) and upper column (10), in an integrated orseparated structure.
 9. The apparatus as described in claim 1, with thefeatures that: The said refrigerant has a boiling point lower than orequal to that of methane under the standard atmospheric pressure, and isa mixture formed by one or a number of gases including methane,nitrogen, argon, helium and hydrogen.
 10. The apparatus as described inclaim 1, with the features that: The apparatus of this invention is alsoapplicable to liquefaction of other gases, and boiling point under thestandard atmospheric pressure of the refrigerant used is lower than orequal to that of the corresponding gas to be liquefied.